A geometric formulation of GENERIC stochastic differential equations
Mark A. Peletier, Marcello Seri
TL;DR
This work addresses the lack of coordinate invariance in stochastic GENERIC formulations by introducing a coordinate-free geometric framework for GENERIC SDEs on manifolds. It defines a gGENERIC SDE using a degenerate Poisson structure ${\mathsf J}$, a degenerate co-metric ${\mathsf K}$, a unimodular volume form ${\nu}$, and energy/entropy functionals $E,S$, yielding a generator $L f = {\mathsf J}(dE, df) + {\mathsf K}(dS, df) + \Delta_{\mathcal H} f$ and a Stratonovich SDE driven by horizontal vector fields; the model preserves the Boltzmann-type measure $e^{S}\nu$ and exactly conserves energy almost surely. It shows a consistent reduction to deterministic GENERIC in the zero-noise limit and casts the Fokker-Planck equation as a deterministic GENERIC evolution on an infinite-dimensional manifold, linking stochastic dynamics to coarse-graining and potential quantum extensions. The framework cleanly separates ambient geometry from system-specific data, enabling robust analytic and numerical methods and providing a principled basis for future extensions to coarse-grained and quantum systems.
Abstract
We propose a coordinate-invariant geometric formulation of the GENERIC stochastic differential equation, unifying reversible Hamiltonian and irreversible dissipative dynamics within a differential-geometric framework. Our construction builds on the classical GENERIC or metriplectic formalism, extending it to manifolds by introducing a degenerate Poisson structure, a degenerate co-metric, and a volume form satisfying a unimodularity condition. The resulting equation preserves a particular Boltzmann-type measure, ensures almost-sure conservation of energy, and reduces to the deterministic GENERIC/metriplectic formulation in the zero-noise limit. This geometrization separates system-specific quantities from the ambient space, clarifies the roles of the underlying structures, and provides a foundation for analytic and numerical methods, as well as future extensions to quantum and coarse-grained systems.
